Interface Electronic Structure and Valence Band Dispersion of Bis(1,2,5-thiadiazolo)-p-quinobis(1,3-dithiole) on Polycrystalline Au Electrodes

Author(s):  
Yasuo Nakayama ◽  
Koji Sudo ◽  
Noboru Ohashi ◽  
Satoshi Kera ◽  
Yasuyuki Watanabe
2005 ◽  
Vol 865 ◽  
Author(s):  
Ralf Hunger ◽  
Christian Pettenkofer

AbstractClean and ordered chalcopyrite CuInSe2 surfaces are a precondition for the study of the electronic structure by angle-resolved photoelectron spectroscopy. The preparation of welldefined CuInSe2(001) surfaces by the combination of molecular beam epitaxy and a selenium capping and decapping process is described. The surface structure of CuInSe2 epilayers with different bulk composition is compared and analysed by low-energy electron diffraction.Employing near-stoichiometric surfaces, the valence electronic structure of CuInSe2 was investigated by angle-resolved photoelectron spectroscopy at the synchrotron source BESSY 2. This is the first study of the valence band structure of a copper chalcopyrite semiconductor material by photoelectron spectroscopy. The valence band dispersion along τT, i.e. the [001] direction, was investigated by a variation of the excitation energy from 10 to 35 eV under normal emission, and the band dispersion along τT, i.e. the [110] direction, was analysed by angular scans with hv = 13 eV.The valence bands derived from antibonding and bonding Se4p-Cu3d hybrid orbitals, nonbonding Cu3d states and In-Se hybrid states are clearly indentified. The strongest dispersion is found for the topmost valence band with a bandwidth of ∼0.7 eV from τ to T. From τ to N, the observed dispersion was 0.5 eV. The experimental valence bands are discussed in relation to calculated band structures in the literature.


1997 ◽  
Vol 9 (14) ◽  
pp. 2955-2961 ◽  
Author(s):  
D Brown ◽  
M D Crapper ◽  
K H Bedwell ◽  
M Petty ◽  
J G Smith ◽  
...  

ChemSusChem ◽  
2017 ◽  
Vol 10 (9) ◽  
pp. 2099-2106 ◽  
Author(s):  
Markus Pichler ◽  
Jakub Szlachetko ◽  
Ivano E. Castelli ◽  
Nicola Marzari ◽  
Max Döbeli ◽  
...  

2021 ◽  
Author(s):  
Giorgia Olivieri ◽  
Gregor Kladnik ◽  
Dean Cvetko ◽  
Matthew A. Brown

The electronic structure of hydrated nanoparticles can be unveiled by coupling a liquid microjet with a resonant photoemission spectroscopy.


2021 ◽  
Vol 90 (12) ◽  
Author(s):  
Fumihiko Matsui ◽  
Seiji Makita ◽  
Hiroyuki Matsuda ◽  
Eiken Nakamura ◽  
Yasuaki Okano ◽  
...  

1982 ◽  
Vol 25 (4) ◽  
pp. 351-354
Author(s):  
V. V. Konev ◽  
V. A. Chaldyshev

2001 ◽  
Vol 64 (8) ◽  
Author(s):  
P. A. Shields ◽  
R. J. Nicholas ◽  
F. M. Peeters ◽  
B. Beaumont ◽  
P. Gibart

1994 ◽  
Vol 01 (04) ◽  
pp. 649-653 ◽  
Author(s):  
A.J. PATCHETT ◽  
S.S. DHESI ◽  
R.I.R. BLYTH ◽  
S.D. BARRETT

An intense photoemission feature is observed at a binding energy of ~10 eV in the UV photoemission spectra from the (0001) surfaces of bulk single crystals of rare-earth metals. This emission cannot be explained in terms of ground state electronic structure and we have been unable to attribute its existence to the presence of contamination of the surface. We present some evidence that may indicate its origin lies in the creation, by the photoemission process, of a metastable two-hole final state.


2014 ◽  
Vol 126 (2) ◽  
pp. 511-515 ◽  
Author(s):  
JAKUB SZLACHETKO ◽  
KATARZYNA MICHALOW-MAUKE ◽  
MAARTEN NACHTEGAAL ◽  
JACINTO SÁ

1995 ◽  
Vol 378 ◽  
Author(s):  
Art J. Nelson ◽  
K. Sinha ◽  
John Moreland

AbstractSynchrotron radiation soft x-ray photoemission spectroscopy was used to investigate the development of the electronic structure at the CdS/Cu2Se heterojunction interface. Cu2−xSe layers were deposited on GaAs (100) by molecular beam epitaxy from Cu2Se sources. Raman spectra reveal a strong peak at 270 cm−1, indicative of the Cu2−xSe phase. Atomic force microscopy reveals uniaxial growth in a preferred (100) orientation. CdS overlayers were then deposited in-situ, at room temperature, in steps on these epilayers. Photoemission measurements were acquired after each growth in order to observe changes in the valence band electronic structure as well as changes in the Se3d and Cd4d core lines. The results were used to correlate the interfacial chemistry with the electronic structure and to directly determine the CdS/Cu2−xSe and heterojunction valence band discontinuity and the consequent heterojunction band diagram. These results are compared to the valence band offset (ΔEv) for the CdS/CuInSe2 heterojunction interface.


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